JPS631766B2 - - Google Patents
Info
- Publication number
- JPS631766B2 JPS631766B2 JP54013787A JP1378779A JPS631766B2 JP S631766 B2 JPS631766 B2 JP S631766B2 JP 54013787 A JP54013787 A JP 54013787A JP 1378779 A JP1378779 A JP 1378779A JP S631766 B2 JPS631766 B2 JP S631766B2
- Authority
- JP
- Japan
- Prior art keywords
- source
- transistor circuit
- current
- constant current
- circuit
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
Links
Classifications
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03F—AMPLIFIERS
- H03F1/00—Details of amplifiers with only discharge tubes, only semiconductor devices or only unspecified devices as amplifying elements
- H03F1/30—Modifications of amplifiers to reduce influence of variations of temperature or supply voltage or other physical parameters
- H03F1/301—Modifications of amplifiers to reduce influence of variations of temperature or supply voltage or other physical parameters in MOSFET amplifiers
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03F—AMPLIFIERS
- H03F1/00—Details of amplifiers with only discharge tubes, only semiconductor devices or only unspecified devices as amplifying elements
- H03F1/26—Modifications of amplifiers to reduce influence of noise generated by amplifying elements
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03F—AMPLIFIERS
- H03F1/00—Details of amplifiers with only discharge tubes, only semiconductor devices or only unspecified devices as amplifying elements
- H03F1/34—Negative-feedback-circuit arrangements with or without positive feedback
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03F—AMPLIFIERS
- H03F3/00—Amplifiers with only discharge tubes or only semiconductor devices as amplifying elements
- H03F3/26—Push-pull amplifiers; Phase-splitters therefor
- H03F3/265—Push-pull amplifiers; Phase-splitters therefor with field-effect transistors only
-
- H—ELECTRICITY
- H03—ELECTRONIC CIRCUITRY
- H03F—AMPLIFIERS
- H03F3/00—Amplifiers with only discharge tubes or only semiconductor devices as amplifying elements
- H03F3/30—Single-ended push-pull [SEPP] amplifiers; Phase-splitters therefor
- H03F3/3001—Single-ended push-pull [SEPP] amplifiers; Phase-splitters therefor with field-effect transistors
- H03F3/3044—Junction FET SEPP output stages
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Amplifiers (AREA)
- Junction Field-Effect Transistors (AREA)
Description
【発明の詳細な説明】
本発明はトランジスタ回路に関し特にソース接
地型の電界効果トランジスタ増幅回路に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a transistor circuit, and particularly to a common source type field effect transistor amplifier circuit.
電界効果トランジスタを動作させるためのバイ
アス回路として自己バイアス回路が広く用いられ
ている。第1図にNチヤンネルの接合型デイプレ
ツシヨンFET(電界効果トランジスタ)のソース
接地増幅器に、上記自己バイアス回路を適用した
場合の回路図を示す。 Self-bias circuits are widely used as bias circuits for operating field-effect transistors. FIG. 1 shows a circuit diagram in which the self-bias circuit described above is applied to a common source amplifier of an N-channel junction type depletion FET (field effect transistor).
すなわち、トランジスタQ1のソースと接地間
にはバイアス用ソース抵抗RSが設けられ、ドレ
インには負荷抵抗RDが接続され、ゲート入力が
増幅されてドレイン出力となる。尚、Riは入力
抵抗を示す。 That is, a bias source resistor R S is provided between the source and ground of the transistor Q 1 , a load resistor R D is connected to the drain, and the gate input is amplified and becomes the drain output. Note that Ri indicates input resistance.
かゝる構成において、ドレイン電流IDによりソ
ースは接地に対して正となり、よつてゲートはソ
ースに対して負となり逆方向バイアスが付与され
ることになる。その結果次式が成立する。 In such a configuration, the drain current I D causes the source to be positive with respect to ground, and thus the gate is negative with respect to the source, providing a reverse bias. As a result, the following equation holds true.
VGS=−ID・RS ……(1) こゝにVGSはゲート・ソース間電圧を示す。 V GS = −I D・R S ...(1) Here, V GS indicates the gate-source voltage.
こゝで、Nチヤンネル・デイプレツシヨン型
FETの入出力伝達特性は第2図の曲線A若しく
はBで示す如くなる。この2曲線A、BはFET
の素子のバラツキによる入出力特性(VGS−ID特
性)の変化の一例を示したものであり、ソース抵
抗RSによる動作点の決定が同図にRS線を引くこ
とによつてなされうる。すなわち(1)式からID=−
VGS/RSが得られるから、第2図においてRS線は原
点を通る直線となることが判る。 Here, N channel depression type
The input/output transfer characteristic of the FET is as shown by curve A or B in FIG. These two curves A and B are FET
This figure shows an example of how the input/output characteristics (V GS − ID characteristics) change due to variations in the elements. The operating point based on the source resistance R S can be determined by drawing the R S line in the figure. sell. In other words, from equation (1), I D =−
Since V GS /R S is obtained, it can be seen that the R S line in FIG. 2 is a straight line passing through the origin.
従つて、特性AのFETにて、ドレイン電流ID1
を流すべくRSを決定すれば、FETQ1のドレイン
電位は+VDD−RD・ID1となる。一方、この第1図
の回路において特性BのFETを使用すればドレ
イン電流はID2となり、よつてドレイン電位は+
VDD−RD・ID2となつて大幅に変動することが理解
できる。 Therefore, in a FET with characteristic A, the drain current I D1
If R S is determined to flow, the drain potential of FETQ 1 becomes +V DD −R D ·I D1 . On the other hand, if a FET with characteristic B is used in the circuit shown in Fig. 1, the drain current will be I D2 , and therefore the drain potential will be +
It can be seen that there is a large fluctuation as V DD −R D・I D2 .
その解決方法としてソース抵抗RSを大とすれ
ばRS線の傾斜が小となり、その結果変動幅を小
としうるが、それだけ回路利得が低下する欠点が
ある。更には、RSは信号源抵抗の一部ともなる
ので、これを大とすれば、RSの熱雑音が大とな
つてS/Nの劣化ともなる。このように、ソース
抵抗RSによりFET素子のバラツキを補正してド
レイン電流を制御することは困難となつている。 As a solution to this problem, if the source resistance R S is increased, the slope of the R S line becomes smaller, and as a result, the fluctuation width can be reduced, but this has the disadvantage that the circuit gain decreases accordingly. Furthermore, since R S also becomes a part of the signal source resistance, if it is made large, the thermal noise of R S becomes large and the S/N ratio deteriorates. As described above, it has become difficult to control the drain current by correcting variations in the FET elements using the source resistance R S.
本発明の目的はソース抵抗を極力小とし熱雑音
の影響を軽減すると共に回路利得も大としうるソ
ース接地型のFETトランジスタ回路を提供する
ことである。 An object of the present invention is to provide a source-grounded FET transistor circuit that can minimize the source resistance, reduce the influence of thermal noise, and increase the circuit gain.
本発明の他の目的は電力増幅回路等に用いられ
る出力プツシユプル増幅回路のドライバ段に用い
て好適なソース接地型のFETトランジスタ回路
を提供することである。 Another object of the present invention is to provide a common source type FET transistor circuit suitable for use in a driver stage of an output push-pull amplifier circuit used in a power amplifier circuit or the like.
本発明のトランジスタ回路はソース抵抗を有す
るソース接地型のFET回路であつて、ソース抵
抗にドレイン電流以外の所定電流を供給する定電
流源を付加することを特徴とするものであつて、
この定電流源の電流値をFETのバラツキに起因
する入出力伝達特性の偏差に対応して調整可能に
構成したことを特徴としている。 The transistor circuit of the present invention is a source-grounded FET circuit having a source resistance, and is characterized in that a constant current source is added to the source resistance to supply a predetermined current other than the drain current,
The present invention is characterized in that the current value of this constant current source can be adjusted in response to deviations in input/output transfer characteristics caused by variations in FETs.
本発明のトランジスタ回路をプツシユプル型の
電力増幅回路のドライバ段とした場合には、ソー
スがそれぞれ第1及び第2のソース抵抗を介して
接地され互いにソース接地型動作をなす第1及び
第2のコンプリメンタリFETと、第1及び第2
のソース抵抗にドレイン電流以外の電流をそれぞ
れ供給する第1及び第2の定電流源とを含み、第
1及び第2のFETのドレイン出力をそれぞれプ
ツシユプルトランジスタの制御入力とすることを
特徴としている。 When the transistor circuit of the present invention is used as a driver stage of a push-pull type power amplifier circuit, the sources of the first and second transistors are grounded through the first and second source resistors, respectively, and the transistor circuit of the present invention operates as a common source type. Complementary FET, first and second
a first and a second constant current source that respectively supply a current other than the drain current to the source resistor of the FET, and the drain outputs of the first and second FETs are respectively used as control inputs of the push-pull transistor. It is said that
好ましくは、第1及び第2の定電流源の電流値
をそれぞれ調整してFETの入出力伝達特性の偏
差をカバーし両ドレイン出力電位を等しくするこ
とを特徴とするものである。 Preferably, the current values of the first and second constant current sources are adjusted respectively to cover deviations in the input/output transfer characteristics of the FET and to equalize both drain output potentials.
以下、本発明につき図面を用いて説明する。 Hereinafter, the present invention will be explained using the drawings.
第3図は本発明の一実施例を示す回路図であ
り、第1図と同等部分は同一符号により示されて
いる。本例においては第1図の回路に更に定電流
源1を付加し、ソース抵抗RSへドレイン電流ID以
外に定電流I0を供給するものである。 FIG. 3 is a circuit diagram showing an embodiment of the present invention, and parts equivalent to those in FIG. 1 are designated by the same reference numerals. In this example, a constant current source 1 is further added to the circuit shown in FIG. 1, and a constant current I 0 is supplied to the source resistor R S in addition to the drain current ID .
従つて、次式が成立することが判る。 Therefore, it can be seen that the following equation holds true.
VGS=−(ID+I0)・RS ……(2) この式を変形してIDを求めると次式となる。 V GS = - (I D + I 0 ) · R S ...(2) When this formula is transformed to find I D , the following formula is obtained.
ID=−VGS/RS−I0 ……(3)
(3)式を用いて、電流源1により修正されたRS
線を入出力伝達特性曲線中に描くと第4図の実線
で示す直線となる。この場合、所定の定電流I0で
特性Bを有する素子のドレイン電流をID1になる
ようにソース抵抗RSを選定した場合において、
特性Aを有する素子のドレイン電流をもID1に等
しくするためにはソース抵抗RSはそのまゝにし
ておき、定電流値をI0′に調整して第4図の点線
で示すRS線に平行移動せしめることにより可能
となることが判る。 I D = −V GS /R S −I 0 ...(3) Using equation (3), R S corrected by current source 1
When a line is drawn in the input/output transfer characteristic curve, it becomes a straight line shown by the solid line in FIG. In this case, when the source resistance R S is selected so that the drain current of the element having characteristic B becomes I D1 at a predetermined constant current I 0 ,
In order to make the drain current of the element with characteristic A equal to I D1 , the source resistance R S is left as is, and the constant current value is adjusted to I 0 ' to increase R S as shown by the dotted line in Figure 4. It can be seen that this is possible by moving the line in parallel.
このことは、すなわちソース抵抗RSの電圧降
下をドレイン電流のみでなく(ID+I0)により発
生させて行うものであるから、ソース抵抗RSの
値を小として、修正RS線の傾斜を大としたまゝ、
出力電圧の値をFETのバラツキによらず一定と
しうることを意味する。よつてソース抵抗RSに
よる熱雑音の発生及び利得の低下が抑えられるこ
とになる。 In other words, since the voltage drop across the source resistance R S is caused not only by the drain current but also by (I D + I 0 ), the value of the source resistance R S is set small and the slope of the corrected R S line is Keep it big,
This means that the output voltage value can be kept constant regardless of FET variations. Therefore, generation of thermal noise and decrease in gain due to the source resistance R S can be suppressed.
第5図は第3図の回路をプツシユプル電力増幅
回路2のドライバ段3に適用した場合であり、ゲ
ートが共通接続された互いに相補型のいわゆるコ
ンプリメンタリFETQ1及びQ2は、それぞれソー
ス抵抗RS1及びRS2を介してソースが接地されてお
り、ドレインはそれぞれ負荷抵抗RD1,RD2を介
して正負電源へ接続されている。そして、各ソー
ス抵抗RS1及びRS2へ定電流I01,I02をそれぞれ供
給する定電流源11及び12が設けられており、
各ドレイン出力がプツシユプル増幅回路2を構成
するコレクタ共通のコンプリメンタリSEPP出力
トランジスタQ3,Q4のベース入力となつている。
両トランジスタQ3,Q4のエミツタは抵抗R1,R2
を介して正負電源へそれぞれ接続されている。
尚、RLは負荷を示している。 FIG. 5 shows a case where the circuit of FIG. 3 is applied to the driver stage 3 of the push-pull power amplifier circuit 2, and the so-called complementary FETs Q 1 and Q 2 whose gates are commonly connected are each connected to a source resistor R S1 The source is grounded via R and R S2 , and the drain is connected to the positive and negative power supplies via load resistors R D1 and R D2 , respectively. Constant current sources 11 and 12 are provided to supply constant currents I 01 and I 02 to the respective source resistors R S1 and R S2 , respectively.
Each drain output serves as the base input of complementary SEPP output transistors Q 3 and Q 4 having common collectors and forming the push-pull amplifier circuit 2 .
The emitters of both transistors Q 3 and Q 4 are resistors R 1 and R 2
are connected to the positive and negative power supplies through the terminals.
Note that R L indicates the load.
こゝで、両ソース抵抗RS1,RS2を共に小に等し
く選定した場合、両FETQ1,Q2の特性が大きく
バラツイていても、定電流源11,12の駆動電
流I01及び吸込電流I02の値を適当に選定して、両
ドレイン出力電位の絶対値を等しくすることが可
能となり、第3図に示した回路の効果を有する上
に更に、プツシユプルトランジスタQ3,Q4のベ
ースバイアスを等しくできるから、両トランジス
タQ3,Q4の出力電流に差を生じることなくよつ
てオフセツト出力が生じないという利点がある。 Here, if both source resistances R S1 and R S2 are selected to be equally small, even if the characteristics of both FETQ 1 and Q 2 vary widely, the drive current I 01 and sink current of constant current sources 11 and 12 By appropriately selecting the value of I 02 , it becomes possible to equalize the absolute values of both drain output potentials, and in addition to having the effect of the circuit shown in FIG. 3, push pull transistors Q 3 and Q 4 Since the base biases of both transistors Q 3 and Q 4 can be made equal, there is no difference in the output currents of both transistors Q 3 and Q 4 , which has the advantage that no offset output occurs.
第6図は本発明の他の実施例を示す回路図であ
り、第5図の回路のソース抵抗RS1及びRS2を共通
にして可変抵抗器としたものである。すなわち、
この可変抵抗器Rの可変端子が接地されて、可変
端子の両側の分割抵抗部分がそれぞれRS1,RS2に
相当するものである。 FIG. 6 is a circuit diagram showing another embodiment of the present invention, in which the source resistances R S1 and R S2 of the circuit of FIG. 5 are made common to form a variable resistor. That is,
The variable terminal of this variable resistor R is grounded, and the divided resistance portions on both sides of the variable terminal correspond to R S1 and R S2 , respectively.
こゝで、可変端子を任意の点に選定した場合、
RS2=R−RS1となり、またRS1=α・R(αは係
数)とすればRS2=R−αR=R(1−α)となる。
よつてそれぞれの抵抗の電圧降下は次式となる。 Here, if you select the variable terminal at an arbitrary point,
R S2 =R-R S1 , and if R S1 =α·R (α is a coefficient), R S2 =R-αR=R(1-α).
Therefore, the voltage drop across each resistor is as follows.
ここで両定電流源の電流値は等しくI0に選定さ
れており、両FETのゲート・ソース間電圧を
VGS1,VGS2としている。 Here, the current values of both constant current sources are selected to be equal to I 0 , and the gate-source voltage of both FETs is
V GS1 and V GS2 are used.
従つて、第6図の回路に於ては、両定電流源の
電流I0は共に相等しくしたまゝ、可変抵抗器によ
りVGS1,VGS2の値を反比例的に変化させることが
できるから、ドレイン電流の調整が第5図の電流
源の調整よりも容易となる。ここで、可変抵抗器
は、FETの相対的なバラツキ補正として用い、
また電流I0はFETの絶対的なバラツキ補正として
使用することによつて広範囲の補正が可能となり
量産性に向く。 Therefore, in the circuit shown in Figure 6, while the currents I0 of both constant current sources are kept equal, the values of V GS1 and V GS2 can be changed inversely proportionally using the variable resistor. , adjustment of the drain current becomes easier than adjustment of the current source shown in FIG. Here, the variable resistor is used to compensate for relative variations in the FET,
Furthermore, by using the current I 0 as an absolute variation correction of the FET, a wide range of correction becomes possible, which is suitable for mass production.
第7図は第6図の回路3をプツシユプル増幅器
2と共に用いていわゆるNFB(ネガテイブフイー
ドバツク)アンプとしたものであり、第5,6図
と同等部分は同一符号により示されており、抵抗
R3,R4がNFB回路となつている。 Fig. 7 shows a so-called NFB (negative feedback) amplifier using the circuit 3 of Fig. 6 together with the push-pull amplifier 2. The same parts as in Figs. 5 and 6 are indicated by the same symbols, and the resistors
R 3 and R 4 form the NFB circuit.
尚、可変抵抗器RはFETのVGSを変化せしめて
ドレイン電流IDを等しくするものであり、定電流
の調整はその絶対値を変化せしめてIDのバラツキ
をなくして出力プツシユプルトランジスタのコレ
クタ電流を一定とするものである。また、可変抵
抗器Rは中点オフセツト調整用として、定電流源
は出力トランジスタのアイドル電流設定用として
も用いられる。 The variable resistor R is used to equalize the drain current ID by changing the VGS of the FET, and the constant current is adjusted by changing its absolute value to eliminate variations in the output push-pull transistor. The collector current of is kept constant. Further, the variable resistor R is used for adjusting the midpoint offset, and the constant current source is also used for setting the idle current of the output transistor.
第8図の回路は、第6,7図の回路における可
変抵抗器Rに対して更に抵抗R5を並列に付加し
たものである。一般に可変抵抗器Rはその全抵抗
値が非常に小さいものはコスト的に高いものであ
るから、この可変抵抗器Rとしてある程度抵抗値
の大きなものを使用してコスト低減を図り、かつ
等価的に小さな抵抗とする回路である。 The circuit of FIG. 8 has a resistor R5 added in parallel to the variable resistor R in the circuits of FIGS. 6 and 7. Generally speaking, a variable resistor R with a very small total resistance value is expensive in terms of cost, so it is possible to reduce the cost by using a variable resistor R with a relatively large resistance value. This is a circuit with small resistance.
すなわちaに示す如く可変抵抗器Rの上側及び
下側抵抗をそれぞれαR、(1−α)Rとし、bに
示すようにいわゆる△−Y(デルタ・スター)変
換を行えば、次式が得られる。 That is, if the upper and lower resistances of the variable resistor R are αR and (1-α)R, respectively, as shown in a, and the so-called △-Y (delta star) conversion is performed as shown in b, the following equation is obtained. It will be done.
従つて、等価的なRa,Rb及びRcをいずれも小
としうることが判る。 Therefore, it can be seen that the equivalent values of Ra, Rb and Rc can all be made small.
以上述べた如く、本発明によればFET素子の
バラツキを、ソース抵抗を大とすることなく補正
できるので、回路利得の低減やS/Nの劣化がな
い。またプツシユプルパワーアンプのドライバ段
に本発明の回路を用いれば、上述の効果の他に更
にオフセツト電流の削減も可能となる利点があ
る。 As described above, according to the present invention, variations in FET elements can be corrected without increasing the source resistance, so there is no reduction in circuit gain or deterioration of S/N. Furthermore, if the circuit of the present invention is used in the driver stage of a push-pull power amplifier, there is an advantage that in addition to the above-mentioned effects, it is also possible to further reduce offset current.
第1図は従来の回路例を示す図、第2図は
FET素子の特性を示す図、第3図は本発明の一
実施例を示す図、第4図は第3図の回路の特性を
示す図、第5図は第3図の回路の一応用例を示す
図、第6図は本発明の他の実施例を示す図、第7
図は第6図の回路の一応用例を示す図、第8図a
は本発明の別の実施例を示す図、bはその等価回
路図である。
主要部分の符号の説明、1……定電流源、Q1,
Q2……FET、RS……ソース抵抗。
Figure 1 shows an example of a conventional circuit, and Figure 2 shows an example of a conventional circuit.
FIG. 3 is a diagram showing the characteristics of the FET element, FIG. 3 is a diagram showing an embodiment of the present invention, FIG. 4 is a diagram showing the characteristics of the circuit in FIG. 3, and FIG. 5 is an example of an application of the circuit in FIG. 3. Figure 6 is a diagram showing another embodiment of the present invention, Figure 7 is a diagram showing another embodiment of the present invention.
The figure shows an example of the application of the circuit in Figure 6, and Figure 8a.
1 is a diagram showing another embodiment of the present invention, and b is an equivalent circuit diagram thereof. Explanation of symbols of main parts, 1...constant current source, Q 1 ,
Q 2 ...FET, R S ...source resistance.
Claims (1)
トランジスタ回路であつて、前記ソース抵抗にド
レイン電流以外に電流値が調整自在に成された定
電流源により所定電流を供給するよう構成し、前
記電界効果トランジスタの入出力特性のバラツキ
を上記定電流源より供給される電流値を調整する
ことで補正可能としたことを特徴とするトランジ
スタ回路。 2 ソースがそれぞれ第1及び第2のソース抵抗
を介して接地され互いにソース接地型動作を行う
第1及び第2のコンプリメンタリ電界効果トラン
ジスタを有するトランジスタ回路であつて、前記
第1及び第2のソース抵抗に各々のドレイン電流
以外に電流値が調整自在に成された第1及び第2
の定電流源により所定電流を供給するよう構成
し、前記電界効果トランジスタの各入出力特性の
バラツキを上記第1及び第2の定電流源より供給
される電流値を調整することで補正可能としたこ
とを特徴とするトランジスタ回路。 3 前記第1及び第2の定電流源の電流はその絶
対値が共に相等しく選定されており、前記第1及
び第2のソース抵抗は可変端子が接地された可変
抵抗器の分割抵抗部分よりそれぞれ構成されてい
ることを特徴とする特許請求の範囲第2項記載の
トランジスタ回路。 4 前記第1及び第2のソース抵抗は更に前記可
変抵抗器の両端に接続された固定抵抗素子より構
成されていることを特徴とする特許請求の範囲第
3項記載のトランジスタ回路。 5 前記可変抵抗器の全抵抗は前記固定抵抗素子
の抵抗よりも極めて大に選定されていることを特
徴とする特許請求の範囲第4項記載のトランジス
タ回路。[Scope of Claims] 1. A source-grounded field effect transistor circuit having a source resistor, which supplies a predetermined current to the source resistor in addition to the drain current by a constant current source whose current value is adjustable. 1. A transistor circuit comprising: a transistor circuit configured to be capable of correcting variations in input/output characteristics of the field effect transistor by adjusting a current value supplied from the constant current source. 2. A transistor circuit comprising first and second complementary field effect transistors whose sources are grounded via first and second source resistors, respectively, and which mutually perform common source type operation, wherein the first and second sources The first and second resistors each have a current value that can be adjusted in addition to the respective drain currents.
A constant current source is configured to supply a predetermined current, and variations in each input/output characteristic of the field effect transistor can be corrected by adjusting the current values supplied from the first and second constant current sources. A transistor circuit characterized by: 3 The absolute values of the currents of the first and second constant current sources are selected to be equal to each other, and the first and second source resistances are selected from a dividing resistance portion of a variable resistor whose variable terminal is grounded. 3. The transistor circuit according to claim 2, wherein the transistor circuit is configured as follows. 4. The transistor circuit according to claim 3, wherein the first and second source resistors further include fixed resistance elements connected to both ends of the variable resistor. 5. The transistor circuit according to claim 4, wherein the total resistance of the variable resistor is selected to be much larger than the resistance of the fixed resistance element.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1378779A JPS55107307A (en) | 1979-02-08 | 1979-02-08 | Transistor circuit |
| US06/117,590 US4356453A (en) | 1979-02-08 | 1980-02-01 | Reduced noise-improved gain transistor circuit |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1378779A JPS55107307A (en) | 1979-02-08 | 1979-02-08 | Transistor circuit |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS55107307A JPS55107307A (en) | 1980-08-18 |
| JPS631766B2 true JPS631766B2 (en) | 1988-01-14 |
Family
ID=11842952
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1378779A Granted JPS55107307A (en) | 1979-02-08 | 1979-02-08 | Transistor circuit |
Country Status (2)
| Country | Link |
|---|---|
| US (1) | US4356453A (en) |
| JP (1) | JPS55107307A (en) |
Families Citing this family (13)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5748718U (en) * | 1980-09-04 | 1982-03-18 | ||
| JPS6016022A (en) * | 1983-07-08 | 1985-01-26 | Fujitsu Ltd | Complementary logic circuit |
| JPS6016021A (en) * | 1983-07-08 | 1985-01-26 | Fujitsu Ltd | Complementary logic circuit |
| US4578629A (en) * | 1983-09-09 | 1986-03-25 | Westinghouse Electric Corp. | Monolithic microwave "split load" phase inverter for push-pull monolithic FET amplifier circuits |
| US4667256A (en) * | 1985-11-25 | 1987-05-19 | Eastman Kodak Company | Circuit for electro-optic modulators |
| BE1000333A7 (en) * | 1987-02-20 | 1988-10-25 | Bell Telephone Mfg | Correction chain for a amplifier. |
| FR2708807B1 (en) * | 1993-08-06 | 1995-09-29 | Bourgeois Christian | Electrical signal amplifier. |
| US5939940A (en) * | 1997-06-11 | 1999-08-17 | Stmicroelectronics, Inc. | Low noise preamplifier for a magnetoresistive data transducer |
| US6175279B1 (en) * | 1997-12-09 | 2001-01-16 | Qualcomm Incorporated | Amplifier with adjustable bias current |
| AU2002214206A1 (en) * | 2000-12-08 | 2002-06-18 | Eugene Sergeyevich Aleshin | Differential amplifier |
| US7471151B2 (en) * | 2007-05-14 | 2008-12-30 | Trendchip Technologies Corp. | Circuits for quiescent current control |
| JP4469017B1 (en) * | 2009-07-27 | 2010-05-26 | 邦彦 日比 | Electrical amplification circuit |
| EP3029830A1 (en) * | 2014-12-05 | 2016-06-08 | Centre National De La Recherche Scientifique | Balun device with GFET transistors |
Family Cites Families (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3924198A (en) * | 1971-08-12 | 1975-12-02 | Tektronix Inc | Transistor amplifier having single control to simultaneously adjust level input resistance and input voltage |
| JPS5818333Y2 (en) * | 1974-06-19 | 1983-04-14 | 株式会社東芝 | Zoufuku Cairo |
| JPS5853521B2 (en) * | 1974-11-15 | 1983-11-30 | ソニー株式会社 | Denryokuzo Fuku Cairo |
| GB1518961A (en) * | 1975-02-24 | 1978-07-26 | Rca Corp | Amplifier circuits |
| US4086542A (en) * | 1976-02-12 | 1978-04-25 | Nippon Gakki Seizo Kabushiki Kaisha | Complementary push-pull amplifier |
-
1979
- 1979-02-08 JP JP1378779A patent/JPS55107307A/en active Granted
-
1980
- 1980-02-01 US US06/117,590 patent/US4356453A/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| US4356453A (en) | 1982-10-26 |
| JPS55107307A (en) | 1980-08-18 |
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